JP2008034459A - Solid laser oscillator - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To obtain a solid laser oscillator equipped with a solid laser medium having a low single path absorption rate which can realize a high excitation light effective absorbing rate, and realize miniaturization and high output. <P>SOLUTION: The device comprises a resonator 3 in which both end surfaces 4a, 4b of the solid laser medium 4 work as a resonation mirror for exciting an excitation light 7. The exciting means 2 outputs a laser beam having two or more longitudinal modes as the excitation light 7, and inputs it into the solid laser medium 4 so that it can resonate in the resonator 3. <P>COPYRIGHT: (C)2008,JPO&INPIT

Description

  The present invention relates to a solid-state laser oscillation device, and more particularly to a solid-state laser oscillation device capable of high-efficiency operation.

Conventionally, solid-state laser devices using a solid-state laser medium in which a semiconductor laser (LD) is used as an excitation light source and rare earth ions (or transition metal ions) are added to a host have been actively developed. Most of these are solid-state lasers in which neodymium (Nd) is the active ion, and these ions are added to host crystals (or glass) such as yttrium, aluminum, garnet (Y ₃ Al ₅ O ₁₂ ) and yttrium vanadate (YVO ₄ ). Crystal (solid laser medium) is used. In this case, the absorption coefficient α of the excitation light is relatively high (5 to 30 cm ⁻¹ ), and the optical power of the excitation light from the LD can be substantially absorbed with a crystal length (medium length) d of several mm. Here, the single-pass absorptance η _abs in the solid-state laser medium is expressed by the following equation (1).

η _abs = 1−exp (−αd) (1)
For example, with Nd: YVO ₄ (concentration at 1 at%), an excitation light absorption coefficient α = 30 cm ⁻¹ (excitation wavelength 808.9 nm) is obtained, and at a crystal length of 1 mm, the single-pass absorption η _abs is as high as 95%. Reach. That is, the excitation power can be efficiently absorbed with a crystal length of 1 mm. Nd: YAG (concentration 1 at%) has an excitation light absorption coefficient α = 5 cm ⁻¹ (excitation wavelength 808 nm), and thus a single-pass absorptivity η _abs = 63% can be obtained with a crystal length of about 2 mm. In general, increasing the absorption rate of pumping light is essential for improving the overall efficiency (efficiency from electrical input to optical output) of a high solid-state laser device. In addition, since the pumping light can be absorbed with a short crystal length, a compact LD-pumped solid state laser device can be realized.

On the other hand, in a solid-state laser medium having a low absorption coefficient, the single-pass absorption rate may be remarkably reduced to about 1 to 20% when the crystal length is about several millimeters. For example, when performing hot band excitation (excitation wavelength: 885 nm) with Nd: YAG, the absorption coefficient α is 1.6 cm ⁻¹ , and a 1 mm long crystal has about 15% absorption. Further, in the Ti: Sapphire laser crystal (titanium ion-added sapphire solid laser medium), the absorption coefficient α = 0.6 cm ⁻¹ (excitation wavelength 532 nm), the crystal length 2 mm, the absorption rate η _abs = 11%, and the crystal length 3 mm. Absorption rate η _abs = 16%, very low. Even in a medium having a small absorption coefficient α, if the crystal length d is increased so that the product αd of the absorption coefficient and the crystal length is 2.3 or more, the single-pass absorption rate η _abs > 90% can be increased. However, there is a disadvantage that the cost increases because the crystal becomes large.

Even when the absorption coefficient is relatively high, when quasi-three-level laser oscillation is performed, extending the crystal length d leads to self-absorption of the laser oscillation light and thus an increase in the oscillation threshold, and therefore should be avoided as much as possible. For example, Nd: YAG 946 nm oscillation ( ⁴ F _3/2 → ⁴ I _9/2 ) and Yb: YAG ( ² F _5/2 → ² F _7/2 ) are quasi-three-level systems. It is difficult to achieve both high absorption and low oscillation threshold. Nd: besides YAG also has many laser crystal exhibiting a quasi-three-level system lasing, Pr: blue oscillation at _{YLF (LiYF 4) (480nm,} 3 P 0 → 3 H 4), Pr: in YAG Blue oscillation (488 nm, ³ P ₀ → ³ H ₄ ), blue oscillation at Tm: YLF (482 nm, ¹ G ₄ → ³ H ₆ ), green oscillation at Er: YLF (551 nm, ⁴ S _3/2 → ⁴ Visible light emission such as I _15/2 ) corresponds to quasi-three-level laser oscillation.

Conventionally, some ideas for increasing the absorption rate of excitation light have been proposed. For example, the most simple and often used method is to double-pass the excitation light by turning it back with a mirror provided on the crystal end face or outside (Non-patent Document 1). In this case, the absorption length is twice the crystal length, and the absorption rate is also improved. However, when the absorption coefficient is very low, the effect of thinning the absorption length by about twice is often small. For example, in the previous Nd: YAG hot band excitation, even if the medium length L is increased from 1 mm to 2 mm, η _abs = 27% is approximately doubled, but it is still very low. Further multipath is difficult with a simple optical system.

  On the other hand, a method of multi-passing excitation light using image transfer (image relay) while shifting the axis has been realized. In fact, an optical system that allows a thin disk type Yb: YAG crystal (thickness 0.2 to 0.5 mm) to pass 16 times has been proposed (see Non-Patent Document 2). In this case, however, a very complicated optical system must be arranged with a precise alignment.

  The above example is a case where the excitation light is treated as incoherent light. On the other hand, as an example of using the coherence (coherence) of a pump laser, a resonance effect by an external resonator is used by using a semiconductor laser oscillating with a narrow line width and a single frequency (single longitudinal mode). Things have been proposed and proven. In this case, the oscillation frequency of the pump laser is tuned to the longitudinal mode of the external resonator by temperature or current control, and the resonance state with respect to the pump laser in the external resonator is maintained. The laser crystal is disposed in the external resonator, and the excitation light reciprocates in the external resonator multiple times. As a result, even if the single-pass absorptance of the laser crystal is low, the same effect can be obtained as when the absorption length has been extended to about 10 to 100 times, and the excitation light is efficiently absorbed (non-patented) Documents 3 and 4 and Patent Document 1).

  In the conventional example described in Non-Patent Document 3, as shown in FIG. 14, a single frequency oscillation semiconductor laser (wavelength 810 nm) is used as an excitation light source 101, and an Nd: YAG crystal 102 is excited. The rear side (LD side) 102a of the Nd: YAG crystal 102 and the output mirror 103 form a resonator for the laser oscillation light 108 and, at the same time, operate as an external resonator for the excitation light 107. The Nd: YAG rear side 102a is highly reflective to the laser oscillation light 108 and partially reflected (reflectance 85%) to the 810 nm excitation light 107, and the output mirror 103 is partially reflective to the laser oscillation light 108. (99.5%), and the excitation light 107 is highly reflective. The resonator length was 10 mm. The Nd: YAG crystal 102 has a thickness of 0.3 mm and an Nd concentration of 1 at%. For an excitation power of 10 mW, 1 mW (wavelength 946 nm) is obtained as the output power of the output light 109. Single-pass absorption is not described but can be estimated at 15%. In this example, 946 nm oscillation is a quasi-three level system, and taking a single-pass absorption higher will increase self-absorption loss due to the lower laser level, resulting in lower oscillation efficiency. is doing.

  In Non-Patent Document 4 and Patent Document 5, 946 nm oscillation is realized using the same Nd: YAG crystal. As shown in FIG. 15, the end face of the laser crystal 105 having a thickness of 0.33 mm is used as a resonator mirror to constitute a resonator for both the excitation light 107 and the laser oscillation light 108. Although not shown, a stable operation is realized by providing a wavelength tuning circuit. In this example, a 946 nm oscillation 109 with an output of 30 mW is obtained for an excitation power of 60 mW. Single pass absorption was 18%.

In the conventional example shown in FIGS. 14 and 15, a single frequency (single longitudinal mode) continuous oscillation LD is used as an excitation light source. However, it is difficult to increase the output of a single frequency oscillation pump laser. In order to oscillate at a single frequency, it is necessary to provide an etalon, diffraction grating and distributed feedback (DFB) structure in the resonator, oscillate only the desired laser oscillation frequency, and incur losses to other frequencies. In many cases, the output of the excitation laser beam is reduced. This inevitably leads to a reduction in the output of the solid-state laser using this pump laser. In general, the output of a single frequency oscillation semiconductor laser is limited to about 10 mW to 100 mW.
US Pat. No. 5,048,047 T.Taira et al., IEEE J. Selected Topics on Quantum Electronics vol.3 No.1 (1997) pp.100-104. C. Stewen et al., IEEE J. Selected Topics on Quantum Electronics vol.6 No.4 (2000) pp.650-657. JP Cuthbertson et al., Optics Letters vol.16 no.6 (1991) pp.396-398. WJ Kozlovsky et al., IEEE J. Quantum Electron. Vol.28 no.4 (1992) pp.1139-1141. T. Skettrup, Journal of optics A: Pure and Applied Optics vol.2 (2000) pp. 546-549.

  As described above, conventionally, in order to increase the effective absorption rate for a solid laser medium having a low single-pass absorption rate, (1) a multi-pass excitation optical system is used, and (2) a single frequency with a narrow line width is used. Two methods have been proposed or realized in which absorption enhancement by an external resonator is performed using a pump laser.

  However, the method (1) has a problem that the pumping optical system becomes extremely complicated or large, and the method (2) reduces pumping power by narrowing the pumping light and cannot increase the laser output. There is a problem, and a compact and high-power solid-state laser device has not been realized.

  The present invention has been made in view of the above circumstances, and provides a small-sized and high-power solid-state laser oscillation device while realizing a high effective absorption rate for a solid-state laser medium having a low single-pass absorption rate. With the goal.

The coherence length Lc of the laser light is given by the following equation (2) as a function of the spectral line width Δν in consideration of the Lorentz type spectral distribution.

Where c: speed of light, Δν: spectral line width (frequency width) of the light source. (See (2) in Non-Patent Document 5, or A. Yariv, "Basics of Optoelectronics", Chapter 10, Original Book 3rd Edition, Maruzen)
In general, since the spectral line width of the single frequency continuous oscillation LD is about 100 kHz to 10 MHz, the coherence length in that case can be very long as Lc = 9.5 m (10 MHz) to 950 m (100 kHz). For this reason, in the laser device of the report example (external resonator resonator length <1 cm), the excitation light effectively reciprocates completely inside the external resonator as coherent light. A strengthening effect can be expected.

  On the other hand, the present inventor has found from the above formula (2) that the spectral line width of the pumping light necessary for realizing the high absorption rate of the pumping light is a function of the resonator length of the external resonator and the desired effective absorption rate. Therefore, it has been found that the pump laser does not have to oscillate at a single frequency with a narrow line width. Further, for example, a Fabry-Perot LD of a multi-longitudinal mode, which is not a single longitudinal mode, can oscillate output power from several hundred mW to about 1 W.

The present invention has been made on the basis of the knowledge obtained by the inventor, and the solid-state laser oscillation device of the present invention includes a solid-state laser medium to which rare earth ions or transition metal ions are added, and the solid-state laser medium disposed therein. A solid-state laser oscillation device comprising: a first resonator for laser-oscillating output light from the solid-state laser medium; and excitation means for outputting excitation light for exciting the solid-state laser medium.
Both end surfaces of the solid-state laser medium constitute a second resonator that functions as a resonance mirror that resonates the excitation light,
The excitation means outputs laser light having two or more longitudinal modes as the excitation light and having a coherence length equal to or greater than the resonator length of the second resonator, and resonates in the second resonator. In this way, the solid-state laser medium is input.

  In the solid-state laser oscillation device of the present invention having the above-described configuration, the coherence length of the pumping light can be shortened compared to the conventional technique using the single-frequency oscillation pumping light with a narrow line width, and the coherence length is 9.5 m (10 MHz). It can be as follows.

  The solid-state laser oscillation device of the present invention is suitable when the solid-state laser medium having an absorption rate of 40% or less, more preferably 20% or less, and even 10% or less by a single pass is used as the solid-state laser medium. .

The solid-state laser oscillation device of the present invention has an excitation light intensity reflectance R _{1 of} an input mirror that introduces the excitation light into the resonator among the resonance mirrors constituting the second resonator.

Where R _m : product of excitation light intensity reflectance of mirrors other than the input mirror constituting the second resonator and propagation efficiency in the resonator circulation, γ = αd cos θ: excitation per circulation in the solid-state laser medium Optical field attenuation coefficient, d: medium length of the solid-state laser medium, α: absorption coefficient of the pumping light in the solid-state laser medium, θ: angle of incidence on the solid-state laser medium, L: resonance of the second resonator Device length, Lc: It is desirable to satisfy the coherence length of the excitation light.

When the second resonator is a ring type resonator composed of a plurality of resonance mirrors, R _m represents the product of the excitation light intensity reflectance and the circular propagation efficiency of all the mirrors other than the input mirror. L is the round trip resonator length.

  It is desirable that the solid-state laser medium emits visible light. Moreover, it is desirable that the excitation means includes a GaN-based semiconductor laser. Examples of the GaN semiconductor laser include a GaN semiconductor laser, an InGaN semiconductor laser, and an AlGaN semiconductor laser.

  Furthermore, it is desirable that both end faces of the solid-state laser medium also constitute the first resonator.

  A non-linear medium that is a wavelength conversion element that converts the wavelength of oscillation light from the solid-state laser medium may be provided in the first resonator. The nonlinear medium may be a second harmonic generation nonlinear medium that converts the wavelength of the oscillation light from the solid-state laser medium into a second harmonic, and the non-linear medium may include the excitation light and the oscillation light from the solid-state laser medium. A nonlinear medium that generates a sum frequency or a difference frequency may be used.

A second solid-state laser oscillation device of the present invention includes a solid-state laser medium to which rare earth ions or transition metal ions are added, a nonlinear medium that is a wavelength conversion element that converts the wavelength of oscillation light from the solid-state laser medium, An excitation means for outputting excitation light for exciting the solid-state laser medium,
One end face of the solid-state laser medium and one end face of the nonlinear medium are joined,
The other end face of the solid-state laser medium and the other end face of the nonlinear medium constitute a resonator that resonates both the oscillation light and the excitation light.
The solid-state laser medium so that the excitation means outputs laser light having two or more longitudinal modes as the excitation light and having a coherence length greater than or equal to the resonator length of the resonator, and resonates in the resonator. It is a thing characterized by being input into.

  In the solid-state laser oscillation device of the present invention having the above-described configuration, the coherence length of the pumping light can be shortened compared to the conventional technique using the single-frequency oscillation pumping light with a narrow line width, and the coherence length is 9.5 m (10 MHz). It can be as follows.

  In the solid-state laser oscillation device of the present invention, it is preferable that the excitation unit and the solid-state laser medium are mounted in the same package. In this case, it is desirable that the excitation means and the solid-state laser medium are held by a single support or a bonded and integrated support.

  Furthermore, the solid-state laser oscillation device of the present invention preferably includes temperature adjusting means for adjusting the temperature of the excitation means and the solid-state laser medium.

  In the solid-state laser oscillation device of the present invention, both end faces of the solid-state laser medium constitute a second resonator that functions as a resonance mirror that resonates the excitation light, and the excitation means includes two or more excitation lights. A laser beam having a longitudinal mode and a coherence length equal to or greater than the resonator length of the second resonator is output and input into the second resonator, and a plurality of excitation lights pass through the solid-state laser medium. Since it resonates so as to reciprocate once and again, even in a solid-state laser crystal having a low single-pass absorptance, the effective absorptance can be increased, so that highly efficient operation is possible.

  Compared with the case where longitudinal single mode laser light is used as the excitation light, the structure of the excitation means can be reduced in size, and the excitation light can be increased in output, so that the entire apparatus is small and A high-power solid-state laser oscillation device and solid-state laser amplification device can be configured. Since the etalon effect by the solid-state laser medium is used, it is not necessary to use the band narrowing means for narrowing the laser beam from the semiconductor laser as the pumping means, and the apparatus can be further downsized.

  In the solid-state laser oscillation device of the present invention, as the single-pass absorptance is as small as 40% or less, 20% or less, and further 10% or less, the effect of increasing the efficiency can be obtained remarkably.

  Embodiments of the present invention will be described below.

  FIG. 1 shows a schematic configuration of the solid-state laser oscillation device 1 according to the first embodiment of the present invention. The solid-state laser oscillation device 1 includes an excitation laser 2 that is excitation means for exciting a solid-state laser medium (solid-state laser crystal), a solid-state laser crystal 4 that is coated on both end faces, and excitation light from the excitation laser 2. 7 has a temperature controller 5 (hereinafter referred to as controller 5) which is a temperature adjusting means for detecting the resonance state 7 and applying feedback to the excitation laser 2. The resonance state is conceptually a state in which the frequency of the pumping light and the frequency of the external resonator coincide with each other and the phase is matched, but actually the state in which the reflected light 7 ′ is minimized is resonated. Judge as the state.

Here, the rear side end face 4a and the output side end face 4b of the laser crystal 4 are respectively coated with predetermined coatings to form high reflection mirrors or partial reflection mirrors for the wavelengths of the excitation light 7 and the oscillation light 8, respectively. and the side end surface 4a (referred to as the mirror M _1.) and (referred to as a mirror M _2.) the output side end face 4b, the cavity 3 for resonating both optical excitation light 7 and oscillation light 8 is formed.

The controller 5 adjusts the temperature by receiving and monitoring the reflected light 7 ′ obtained by reflecting the excitation light 7 from the mirror M ₁ with the half mirror 10 by the light receiving element 6. Then, a cooling means such as a Peltier element (not shown) provided in the excitation laser 2 is controlled. However, it is sufficient that the temperature of the excitation laser 2 and / or the laser crystal 4 can be adjusted.

  The excitation laser 2 outputs laser light having two or more longitudinal modes as the excitation light 7 and inputs it to the solid-state laser crystal 4 so as to resonate in the resonator 3, as shown in FIG. A semiconductor laser 11, a collimating lens 12 that collimates the excitation light from the semiconductor laser 11, a wavelength selection filter 13 that narrows the spectral width of the collimated excitation light, and a total reflection mirror 14. It is composed of In FIG. 2, excitation light 7 output to the outside (toward the half mirror 10) is schematically represented by an arrow, and an optical system for inputting to the solid-state laser crystal 4 is not shown. Furthermore, in order to narrow the spectral width of the output light from the semiconductor laser 11, further narrowing means such as an external resonator structure and a diffraction grating, an etalon, etc. may be provided. It is not necessary to narrow the spectral width of the laser beam output from the laser beam 11 so much. The wavelength selection filter 13 is not essential.

In the present embodiment, the laser crystal 4 is Nd: YAG (Nd concentration 0.1 at%), and 946 nm quasi-three-level oscillation is performed. The crystal length d of the laser crystal 4 was 0.5 mm, and the absorption coefficient α of excitation light was 0.5 cm ⁻¹ . The absorptance of the excitation light 7 is η _abs = 1−exp (αd) = 2.5% in a single pass. Here, the resonator length L is equal to the crystal length d, 0.5 mm, and the wavelength of the excitation light 7 is 810 nm.

At this time, when the coherence length Lc of the excitation light is changed from 0 mm (incoherent state) to 100 mm, the effective absorptance of the solid-state laser crystal 4 depends on the excitation light intensity reflectance R ₁ of the input mirror M ₁ . The calculation results are shown in FIG. 3 (in FIG. 3, the coherence length Lc from the top is 100 mm, 50 mm, 5 mm, 2 mm, 1 mm, 0.5 mm, 0 mm). However, the scattering loss in the resonator 3 was ignored because it was sufficiently smaller than the single-pass absorption. The excitation light intensity reflectance of the output mirror M ₂ was R ₂ = 1. The calculation method was based on Fabry-Perot interferometer theory with absorption (T. Skettrup, Journal of Optics A: Pure and Applied Optics vol.2 (2000) pp. 546-549). The optical field of the coherent component reflected from the resonator is written as the following equation (3) in consideration of the coherence length. However, the spatial mode is assumed to be a plane wave. The first term is the reflection at the mirror M ₁ , and the second term is the component through which the excitation light that has reciprocated once passes through the mirror M ₁ (including the effect of reducing the coherent component due to absorption and coherence length, and the phase difference due to rotation). In the same manner, components that circulate many times are added together.

However, E _in: incident electrical field, r _1: the excitation light field reflectivity of the input mirror M _1, t _1: the excitation light field transmission of the input mirror _{M 1, r m = r 2} r 3 (1-E L): The product of the electric field reflectivity of all the mirrors other than the input mirror and the propagation efficiency of the resonator around the resonator = the propagation efficiency associated with the resonator around the input mirror, r ₂ : the electric field reflectivity of the excitation light of the mirror M ₂ , r ₃ : Excitation light electric field reflectivity of mirror M ₃ , E _L : Electric field scattering loss at resonator round, φ = 2 · 2π / λL: Phase difference per round trip, γ = αdcosθ: Excitation per round at laser crystal Optical electric field attenuation coefficient, L: resonator length, d: crystal length (crystal thickness), θ: crystal incident angle. Similarly, the transmitted coherent electric field, incoherent component optical electric field, and the like can be calculated, and finally the absorption power can be calculated. In the calculation, the phase difference φ = 2pπ (where p is an integer).

In this case, if the coherence length is equal to or greater than the resonator length (0.5 mm), or preferably equal to or greater than the resonator length, preferably approximately twice, the effective absorption rate is enhanced to about 12 to 20 times the single-pass absorption. . It can be seen from FIG. 3 that if the coherence length is 1 mm and the excitation light intensity reflectance R ₁ = 0.5 of the input mirror M ₁ , an effective absorption rate of 56% can be obtained. Further, it is understood that if there is a coherence length (5 mm) about 10 times the resonator length, an absorption rate of 90% or more can be obtained in the vicinity of the excitation light intensity reflectance R ₁ = 0.8. Of course, when the coherence length can be regarded as sufficiently longer than the resonator length (100 times or more = 50 mm or more), if the pumping light intensity reflectance R ₁ is appropriately selected, almost all the pumping power is absorbed ( Here, the scattering loss is ignored).

When the coherence length is sufficiently longer than the resonator length, the value of the excitation light intensity reflectance R ₁ of the mirror M ₁ having the maximum absorption rate is given by the following equation (4). Here, if the scattering loss in the resonator is ignored, R _m is the excitation light intensity reflectance R ₂ of the mirror M ₂ .

However, the enhancement due to the coherent effect is not necessarily expressed only at this value, which means that the vicinity of this value is more desirable. Specifically, a sufficient coherent effect can be obtained within the range of the following formula (5).

  The coherence length of 0.5 mm corresponds to the spectral width Δν = 190 GHz of the laser light that is the excitation light 7 output from the excitation laser. Expressed in terms of wavelength, it is 0.4 nm (at 800 nm wavelength). This wavelength width indicates that there is no need to use a narrow line width DFB laser or an external cavity semiconductor laser. This line width is a value that can be easily achieved, and a reduction in excitation power due to a loss due to the narrowing of the band can be kept low, so that a high output can be achieved. When the excitation laser is provided with an external resonator and a diffraction grating or a wavelength selection filter is inserted, the resonator length is about 5 cm. At this time, the free spectral range is 3 GHz, and not about a single frequency, but about 60 longitudinal modes oscillate.

In the experiment, the Fabry-Perot type semiconductor laser 11 (with free running oscillation with a spectral width of 1 nm) was narrowed using only the wavelength selection filter 12 (transmission bandwidth: 0.5 nm). As a result, oscillation with a spectral width of about 0.04 nm was easily realized. An output of 500 mW and a line width of 20 GHz (800 nm wavelength, coherence length 4.7 mm) were obtained. In the solid-state laser oscillation device 1 shown in FIG. 1 using this as the excitation laser 2, the absorption power is 450 mW (absorption rate 90%), the threshold is 100 mW, and the laser output of the output light 9 is 160 mW (slope efficiency 45%). Obtained at a wavelength of 946 nm. When the resonator for resonating the pumping light is not provided, the absorption power of the pumping light of the laser crystal is 2.5% in a single pass, so the pumping power absorbed is only 12.5 mW. Therefore, the threshold required for oscillation was not exceeded and laser oscillation could not be obtained. If the resonator that resonates the pumping light is not provided, the absorption length required for the 90% absorption rate is 4.6 cm, that is, an excitation path for 92 passes (46 reciprocations) of a 0.5 mm crystal is required. It is very difficult to achieve this without using a resonator. At this time, the resonator configuration was as follows: mirror M ₁ : flat mirror, mirror M ₂ : flat mirror, excitation spot radius at crystal 4 of 72 μm. The following coats were applied to each mirror. Mirror M ₁ : reflectivity 80% for excitation light 7 and high reflection (HR) for 946 nm wavelength, mirror M ₂ : HR for excitation light 7 and reflectivity 99% for 946 nm.

Furthermore, when the crystal thickness is about 0.25 mm, the absorptance decreases to about 1.2%, but the effective absorptance depends on the reflectance R ₁ as shown in FIG. The coherence length required here is 0.25 mm or more, and the spectrum width is remarkably broadened to 0.8 nm (381 GHz). At this level, the Fabry-Perot laser that oscillates in the transverse single mode is only slightly narrowed, or may be used as it is.

  In a specific experiment, an external resonator is provided in a Fabry-Perot semiconductor laser having an output of about 1 W, and a volume Bragg diffraction grating with a 0.5 nm spectral width is inserted to easily realize an oscillation of 0.1 nm. It was confirmed that about 800 mW was obtained. When this was used as an excitation laser and a solid laser crystal having a crystal length (etalon thickness) of 0.25 mm was excited, an effective absorption rate of 80% was obtained, and the laser oscillation efficiency was 40% for an absorption power of 640 mW. , 946 nm light of 250 mW was obtained. In this case, the free spectral range (FSR) determined by the etalon (thickness) at 946 nm wavelength is 600 GHz (spectrum width 1.8 nm), which is wider than the laser gain width 0.5 nm, so laser oscillation is realized in a single longitudinal mode. It was done.

  Thus, when the laser crystal is regarded as an etalon, the finesse is approximately 25 at FSR = 600 GHz. The tuning range required for the resonance needs to be tuned to the resonance width of this etalon = FSR / finesse = 24 GHz. However, according to the present invention, a sufficiently coherent effect can be obtained even in a considerably wider width. This is a practically effective means. Since the tuning range of about half of the FSR is sufficiently possible, the coherent effect can be easily obtained even without strict semiconductor laser temperature adjustment or etalon temperature adjustment. Thus, although FIG. 1 (and the following embodiments) clearly shows a controller 5 for optimal tuning, this is not necessarily a requirement and may be unnecessary in some cases.

When an external resonator that resonates pumping light is provided as in the present invention, it is necessary to tune the oscillation frequency of the pump laser to the external resonator, or conversely, to match the frequency of the external resonator with the pump laser. However, there is a Pound-Drever method as a method for maintaining this. This is a method of detecting the reflected light of the input mirror of the external resonator and finely controlling the resonator length so that it is minimized. In order to the above resonance is established optimally is 1) the spatial mode matching of the pump light and oscillation light, 2) impedance matching (input mirror M ₁ excitation light intensity reflectance R ₁ = the intracavity loss: Formula (Equivalent to (4)) is considered necessary (see the literature (WP Risk et al., “Compact Blue-Green Lasers”, Cambridge University Press, Chapter 4) for more details). For the former, it is sufficient to match the mode of the excitation laser resonator mode of the external cavity, since it is TEM ₀₀ mode with each other, is relatively easy. Specifically, the resonator mode formed by the external resonator is calculated using a ray matrix or the like, and the mode spot diameter and the waist position are calculated. The beam is shaped by an external lens system so that the excitation laser beam is focused at this position and spot diameter. Regarding the latter, as shown in FIG. 3, it has been clarified by the inventor's research that the resonance effect is sufficiently exhibited even in a state in which they are not necessarily perfectly matched.

Even when the single-pass absorption is 10% or more, an increase in absorption can be obtained by the coherent effect of the present invention. FIGS. 5 and 6 show cases where single-pass absorption is 10% (α = 2.1 cm ⁻¹ ) and 20% (α = 4.5 cm ⁻¹ ) (crystal length 0.5 mm). However, it can be seen that the rate of absorption enhancement due to the coherent effect is larger when the single-pass absorption is lower. For example, comparing Fig. 3 and Fig. 5, when the coherence length is 0.5mm, the maximum effective absorption rate is 32% and 43% respectively, and the increase from single-pass absorption is 12 and 4.3 times, respectively. is there. This is because if the single-pass absorption is large, the loss in the external resonator increases, and the number of times the pumping light can circulate also decreases. In other words, this is equivalent to a reduction in the effective resonator finesse.

  If the single-pass absorption is larger than 40%, an absorption of 65% or more can be obtained in a normal double-pass configuration without using an external resonator. Therefore, in the case of a single-pass absorption rate of 40% or less, it can be said that using the present invention is very beneficial because an enhancement of about 2 to 20 times the single-pass absorption can be obtained.

In the above-described embodiment, an example in which an Nd: YAG crystal is used as the laser crystal has been described. However, the present invention can be applied to any other laser crystal. For example, in a Pr: YLF (LiYF ₄ ) crystal, it is excited at a wavelength of 440 nm, and is 639.5 nm ( ³ P ₀ → ³ F ₂ ), 522 nm ( ³ P ₁ → ³ H ₅ ), 480 nm ( ³ P ₀ → ³ H ₄ ) Oscillates. In particular, since the 480 nm oscillation has a quasi-three-level energy structure, the effect of applying the present invention is great. A solid-state laser oscillating device similar to that shown in FIG. 1 was constructed, and the laser beam (output 40 mW) from the 440 nm wavelength GaN semiconductor laser was narrowed to a frequency width of about 100 GHz (wavelength width 0.06 nm). As a result, it was possible to obtain an effective absorption rate of 70% or more for a crystal having a single pass absorption of about 5%. A blue 480 nm oscillation of 1 mW was obtained at an absorption power of 25 mW. In addition, Pr: YAG (488 nm, ³ P ₀ → ³ H ₄ ), Ho: YLF (540 nm, ⁵ S ₂ → ⁵ I ₈ ), Tm: YLF (482 nm, ¹ G ₄ → ³ H ₆ ), Er : Solid laser crystals with visible light emission, such as YLF (551 nm, ⁴ S _3/2 → ⁴ I _15/2 ), have many quasi-three-level oscillations. Can be expected.

  In the solid-state laser oscillation device 1 of the first embodiment, the plane-plane cut solid-state laser crystal 4 is used. However, even if one or both of the end faces of the solid-state laser crystal have a curvature, the solid-state laser crystal 4 is cut. Good. This example is shown in FIG. 7 as the solid-state laser oscillation device 20 of the second embodiment. In the following embodiments, the same components as those in the solid-state laser oscillation device shown in FIG.

  In the solid-state laser oscillator 20 of the second embodiment, as the solid-state laser crystal 24, only one end surface 24a is a flat surface and the other end surface 24b is a curved surface. Different. In this case, for example, when the thermal lens is small, it is possible to form a stable resonator mode with a large curvature (several tens of centimeters to several meters). When the thermal lens is strong, one or both end surfaces are concave. Thus, the thermal lens can be compensated and the resonator can be operated stably. Here, the thermal lens is an optical aberration caused by a temperature gradient according to the excitation distribution in a state where the laser crystal is excited, and is usually referred to as a thermal lens because it exhibits a lens effect.

  Next, a solid state laser oscillator 30 according to a third embodiment of the present invention will be described. FIG. 8 is a diagram showing a schematic configuration of the solid-state laser oscillation device 30. The solid-state laser oscillation device 30 includes a solid-state laser medium (laser crystal) 31 to which rare earth ions or transition metal ions are added, and a non-linear medium (non-linear) that is a wavelength conversion element that converts the wavelength of oscillation light from the laser crystal 31. Crystal) 32 and excitation means for outputting the excitation light 7 for exciting the laser crystal 31.

  The excitation means is the same as the excitation laser 2 of the solid-state laser oscillation apparatus of the first embodiment that outputs laser light having two or more longitudinal modes as excitation light.

One end face 31 b of the laser crystal 31 and one end face 32 a of the nonlinear crystal 32 are joined, and the rear end face 31 a (mirror M ₁ ) that is the other end face of the laser crystal 31 and the output side that is the other end face of the nonlinear crystal 32. A resonator 33 that resonates both the oscillation light 8 and the excitation light 7 is constituted by the end face 32b (mirror M ₂ ).

The pumping light 7 resonates around the external resonator 33 constituted by the mirrors M ₁ and M ₂ and is similar to the apparatus of the first embodiment in that it causes laser oscillation by the laser crystal. However, in this embodiment, the laser oscillation light 8 oscillated is continuously converted to the second harmonic by the nonlinear crystal 32, and the output light 9 is the second harmonic, which is different from the apparatus of the first embodiment.

In the solid-state laser oscillation device 30 of this configuration, Nd: YAG (Nd concentration 0.1 at%) is used as the laser crystal 31, and 946 nm quasi-three-level oscillation is performed. The laser crystal 31 has a crystal length d = 0.5 mm, the absorption coefficient alpha = 0.5 cm ^-1 of the excitation light, the wavelength of the excitation light 7 and 810 nm, using a KNbO ₃ crystal as a nonlinear crystal 32, using the first kind phase matching, the phase of coupling angle 60.5 degrees, KNbO ₃ The experiment was conducted with a crystal length of 2 mm. At this time, when the excitation power was 300 mW, the second harmonic 9 in the blue region (473 nm) was about 70 mW, and very high-efficiency blue light was obtained. At this time, the mirror M ₁ has a reflectance of 80% for the excitation light 7 and a high reflectance (HR) for the oscillation light 8, and the mirror M ₂ has a high reflection for the excitation light 7. A coating with a high reflectance (HR), a high reflectance (HR) with respect to the oscillation light 8 and a non-reflection (AR) with respect to the second harmonic 9 was applied.

  In a solid-state laser oscillation device having the same configuration, a GaN semiconductor laser (440 nm) is used as an excitation light source, and a Pr: YLF crystal is used as the solid-state laser crystal 31 instead of Nd: YAG. Second harmonics were generated, and 240 nm deep ultraviolet light 9 could be obtained. In this case, although the laser output was as low as 0.1 mW, an ultraviolet laser could be realized with a very compact configuration.

  In the solid-state laser oscillation device of the third embodiment, the resonator 33 that resonates both the pumping light 7 and the oscillation light 8 by the rear side end face 31a of the laser crystal 31 and the output side end face 32b of the nonlinear crystal 32 is provided. Although it is configured, since the excitation light 7 only needs to be absorbed by the laser crystal, the excitation light 7 only needs to go around the laser crystal. This example will be described as the solid-state laser oscillator 40 of the fourth embodiment.

FIG. 9 shows a schematic configuration of the solid-state laser oscillator 40 of the fourth embodiment. The present solid-state laser oscillator 40 includes a laser crystal 41 and a nonlinear crystal 42 that generates second harmonics, and is the same as that of the third embodiment in that both are joined at one end face 41b and 42a. However, the difference is that resonators for resonating oscillation light and excitation light are individually configured. Specifically, the rear end face 41a (mirror M ₁ ) and the output end face 41b (mirror M ₂ ) of the laser crystal 41 constitute a resonator 43 that resonates the excitation light 7, and the rear end face of the laser crystal 41. A resonator 45 that resonates the oscillation light 8 is constituted by 41a (mirror M ₁ ) and the output side end face 42b (mirror M ₃ ) of the nonlinear crystal 42. Each mirror has the following coats. Mirror M ₁ : 80% reflectivity for excitation light 7, high reflectivity (HR) for oscillation light 8, mirror M ₂ : Mirror M ₃ : high reflectivity (HR) for oscillation light 8, and No reflection (AR) for second harmonic.

Thus, if the external resonator 43 (mirror M ₁ -M ₂ ) for the pumping light 7 and the external resonator 45 (mirror M ₁ -M ₃ ) for the oscillating light 8 are separated, the pumping laser 2 is a laser. Since the solid-state laser oscillation device of the fourth embodiment shown in FIG. 9 has only to have a coherence length determined by the length of the crystal, the solid-state laser oscillation device of the third embodiment shown in FIG. The coherence length of the excitation light may be short.

FIG. 10 shows a schematic configuration of the solid-state laser oscillation device 50 of the fifth embodiment. The solid-state laser oscillation device 50 includes a solid-state laser medium (laser crystal) 51 and a nonlinear crystal 52 that generates a sum frequency or a difference frequency of excitation light and oscillation light, and is nonlinear with one end surface 51b of the laser crystal 51. One end face 52a of the crystal 52 is joined. Here, a resonator 53 that resonates both the pumping light 7 and the oscillation light 8 by the rear end face 51a (mirror M ₁ ) of the laser crystal 51 and the output end face 52b (mirror M ₂ ) of the nonlinear crystal 52 is provided. It is configured.

  For example, when Nd: YAG is used as the solid-state laser crystal 51, in the Nd: YAG 1064nm oscillation, in the sum frequency generation of the 809nm excitation light 7 and the 1064nm oscillation light 8, in the blue region of wavelength 459.5nm, in the difference frequency generation, Generation of the mid-infrared region of 3375 nm is possible. 459.5 nm is suitable for various photochemical reactions, displays, and medical biological applications, and 3375 nm has many resonance lines of vibrational transition of molecules, and can be used for chemical substance identification. In the Nd: YAG 946 nm oscillation, the sum frequency (436 nm) and difference frequency (5586 nm) of the excitation light 7 of 809 nm and the oscillation light 8 of 946 nm and the practically useful wavelength band are very compact. Obtained in configuration.

  Next, as the solid-state laser oscillation device 60 of the sixth embodiment, a semiconductor laser package 61 (for example, a can package or a butterfly package) has a configuration substantially similar to that of the solid-state laser oscillation device of the second embodiment described above. An example in which the laser crystal 21 is included is shown in FIG. Taking advantage of the fact that a very thin laser crystal can be used. By making the laser crystal thin (for example, 0.5 mm or less), the spectral width requirement for the excitation light 7 is greatly relaxed. Effective absorption rate can be increased without narrowing the band. Accordingly, here, the excitation laser 2 ′ is composed of only the semiconductor laser 11 and the condenser lens 15. The excitation laser 2 ′ and the laser crystal 21 are mounted on a heat sink 62 as a support, and a solid laser oscillation device having a very compact configuration enclosed in one package 61 can be obtained.

  In each of the above-described embodiments, it has been described that Nd: YAG is mainly used as the solid-state laser medium. Of course, the solid-state laser medium is not limited to this, but a solid-state laser medium to which rare earth ions or transition metal ions are added. If it is. In addition, it can be widely applied to media where the laser oscillation efficiency decreases, such as a laser crystal with a low single-pass absorptivity or a quasi-three-level laser medium, increasing the absorptance increases the self-absorption loss due to the lower laser level. It is.

  In the above-described embodiment, the resonator mainly resonates both the excitation light and the oscillation light. However, the present invention is not limited to this, and a separate resonator is provided for each of the excitation light and the oscillation light. It may be configured.

FIG. 12 shows a schematic configuration of the solid-state laser oscillator 70 of the seventh embodiment. The solid-state laser oscillation device 70 includes an excitation laser 2, a solid-state laser medium 71, and a concave output mirror 72. The rear end face 71a (mirror M ₁ ) of the solid laser medium 71 and the mirror surface 72a (mirror M ₃ ) of the concave output mirror 72 constitute a first resonator 75 that resonates the oscillation light 8, and the solid laser medium The rear end face 71a (mirror M ₁ ) of 71 and the output end face 71b (mirror M ₂ ) constitute a second resonator 73 that resonates the pumping light 7.

  FIG. 13 shows a schematic configuration of the solid-state laser oscillator 80 of the eighth embodiment. In the first resonator 75 of the solid-state laser oscillator 70 of the seventh embodiment, a nonlinear medium 86 that is a second harmonic conversion element that converts the oscillation light 8 from the solid-state laser medium 71 into a second harmonic is provided. The output light 9 oscillates the second harmonic.

  Also in the solid-state laser oscillators of the seventh and eighth embodiments, the excitation light 7 is resonated by the resonator 73 formed by the both end faces 71a and 71b of the solid-state laser medium 71, and reciprocates in the solid-state laser medium 71. The effect of increasing the absorptance of the pumping light 7 in the solid-state laser medium 71 can be obtained, and the pumping laser 2 outputs laser light having two or more longitudinal modes as the pumping light 7 Therefore, the apparatus can be made compact and high in output as compared with a case where a longitudinal single mode excitation laser is provided as an excitation means.

1 is a schematic configuration diagram of a solid-state laser oscillation device according to a first embodiment. Schematic diagram of excitation laser Input mirror reflectivity dependence of effective absorptance in the first embodiment (single pass absorption = 2.5%) Input mirror reflectivity dependence of effective absorption rate in the first embodiment (single-pass absorption = 1.2%) Input mirror reflectivity dependence of effective absorption rate in the first embodiment (single pass absorption = 10%) Input mirror reflectivity dependence of effective absorptance in the first embodiment (single pass absorption = 20%) Schematic configuration diagram of a solid-state laser oscillation apparatus according to the second embodiment Schematic configuration diagram of a solid-state laser oscillation apparatus according to a third embodiment Schematic configuration diagram of a solid-state laser oscillation apparatus according to a fourth embodiment Schematic configuration diagram of a solid-state laser oscillation apparatus according to a fifth embodiment Schematic configuration diagram of a solid-state laser oscillation apparatus according to a sixth embodiment Schematic configuration diagram of a solid-state laser oscillation apparatus according to a seventh embodiment Schematic configuration diagram of a solid-state laser oscillation apparatus according to an eighth embodiment Conventional example (1) Conventional example (2)

Explanation of symbols

1, 20, 30, 40, 50, 60, 70, 80 Solid state laser oscillator 2 Excitation laser 3 Resonator 4 Solid state laser medium (laser crystal)
5 Controller 6 Light-receiving element 7 Excitation light 8 Oscillation light 9 Output light 10 Half mirror M ₁ , M ₂ , M ₃ mirror

Claims (13)

A solid-state laser medium to which a rare earth ion or a transition metal ion is added; a solid-state laser medium disposed therein; a first resonator for oscillating output light from the solid-state laser medium; and the solid-state laser medium. In a solid-state laser oscillation device provided with excitation means for outputting excitation light to be excited,
Both end surfaces of the solid-state laser medium constitute a second resonator that functions as a resonance mirror that resonates the excitation light,
The excitation means outputs laser light having two or more longitudinal modes as the excitation light and having a coherence length equal to or greater than the resonator length of the second resonator, and resonates in the second resonator. As described above, the solid-state laser oscillation apparatus is characterized in that it inputs to the solid-state laser medium.   2. The solid-state laser oscillation device according to claim 1, wherein an absorptance of the solid-state laser medium with respect to the excitation light is 40% or less in a single pass.   2. The solid-state laser oscillation device according to claim 1, wherein an absorptance of the solid-state laser medium with respect to the excitation light is 20% or less in a single pass.   2. The solid-state laser oscillation device according to claim 1, wherein an absorptance of the solid-state laser medium with respect to the excitation light is 10% or less in a single pass. Among the resonant mirrors constituting the second resonator, the excitation light intensity reflectance R _{1 of} the input mirror that introduces the excitation light into the resonator is:

Where R _m : product of excitation light intensity reflectance of mirrors other than the input mirror constituting the second resonator and propagation efficiency in the resonator circulation, γ = αd cos θ: excitation per circulation in the solid-state laser medium Optical field attenuation coefficient, d: medium length of the solid-state laser medium, α: absorption coefficient of the pumping light in the solid-state laser medium, θ: angle of incidence on the solid-state laser medium, L: resonance of the second resonator 5. The solid-state laser oscillation device according to claim 1, wherein the unit length satisfies L c: the coherence length of the excitation light.   6. The solid-state laser oscillation device according to claim 1, wherein the solid-state laser medium emits visible light.   The solid-state laser oscillation apparatus according to claim 1, wherein the excitation unit includes a GaN-based semiconductor laser.   8. The solid-state laser oscillation device according to claim 1, wherein both end faces of the solid-state laser medium also constitute the first resonator. 9.   8. The solid-state laser according to claim 1, further comprising: a nonlinear medium that is a wavelength conversion element that converts a wavelength of oscillation light from the solid-state laser medium in the first resonator. Oscillator. A solid-state laser medium to which rare earth ions or transition metal ions are added, a nonlinear medium that is a wavelength conversion element that converts the wavelength of oscillation light from the solid-state laser medium, and an excitation that outputs excitation light that excites the solid-state laser medium Means and
One end face of the solid-state laser medium and one end face of the nonlinear medium are joined,
The other end face of the solid-state laser medium and the other end face of the nonlinear medium constitute a resonator that resonates both the oscillation light and the excitation light.
The solid-state laser medium so that the excitation means outputs laser light having two or more longitudinal modes as the excitation light and having a coherence length greater than or equal to the resonator length of the resonator, and resonates in the resonator. A solid-state laser oscillation device characterized by being input to   11. The solid-state laser oscillation device according to claim 1, wherein the excitation unit and the solid-state laser medium are mounted in the same package.   12. The solid-state laser oscillation apparatus according to claim 11, wherein the excitation unit and the solid-state laser medium are held by a single support or a bonded and integrated support.   13. The solid-state laser oscillation device according to claim 1, further comprising temperature adjusting means for adjusting the temperature of the excitation means and the solid-state laser medium.

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